Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
6028Ni32   Nickel
J(π)=0+
T1/2=stable
Abundance: 26.223% 15
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -64.472533
(0.000483)
-64.330 0.120
BE 526.846 526.704
BE/A 8.781 8.778
<R2ch>1/2 = 3.8118 ± 0.0016 fm [3]
Charge-density Distribution [6]

β2= 0.000
β3= 0.000
β4= 0.000
β6= 0.000
Excited States[1]
click on a plot to process it
Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-6291.01
β- - decay-6127.95
β+ - decay-3844.85
e-capture-2822.85
1p - decay-9532.41
2p - decay-16896.07
1n - decay-11387.71
2n - decay-20386.98
- - decay-10298.73
β-,n-16186.07
β-,2n-28947.96
β-,d-17380.04
β-,t-23339.08
β--10857.60
β-,n,α-20939.44
EC,p-11097.40
EC,2p-23223.01
EC,α-9986.62
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
 
σ (b)
Capture 2.90
Scattering 0.98
 
μ (nm) Q (b) E* (keV)
+0.2(3)1332
+0.32(6)1332
-0.10(2)1332
B(E2)↑ = 0.0916 ( 16) e2b2,    β 0  = 0.2052 (19)
2

B(E3)↑ = 0.021 ( 4) e2b3,    β 0  = 0.209 (0)
3

  
[1] National Nuclear Data Center, Evaluated Nuclear Structure Data File, https://www.nndc.bnl.gov/ensdf/.
[2] M. Wang, G. Audi, A.H. Wapstra, F.G. Kondev, M. MacCormick, X. Xu, and B. Pfeiffer, Chinese Physics C, 2012, vol. 36, pp. 1603-2014.
[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.
[4] P. Möller, A.J. Sierk, T. Ichikawa, H. Sagawa, Atomic Data and Nuclear Data Tables, 2016, vol. 109-110, pp. 1-204.
[5] N.J. Stone, https://www-nds.iaea.org/publications/indc/indc-nds-0658/; Atomic Data and Nuclear Data Tables, 2016, vol. 111-112, pp. 1–28.
[6] H. de Vries, C.W. de Jager, C. de Vries, Atomic Data and Nuclear Data Tables, 1987, vol. 36, pp. 495-536.
[7] B. Pritychenko, M. Birch, B. Singh, M. Horoi, Atomic Data and Nuclear Data Tables, 2016, vol. 107, pp. 1–139; 2017, vol. 114, pp. 371–374.
[8] T. Kibedi and R.H. Spear, Atomic Data and Nuclear Data Tables, 2002, vol. 80, pp. 35-82.